Symmetric tunnel field effect transistor

ABSTRACT

The present disclosure relates to semiconductor structures and, more particularly, to a symmetric tunnel field effect transistor and methods of manufacture. The structure includes a gate structure including a source region and a drain region both of which comprise a doped VO 2  region.

FIELD OF THE INVENTION

The present disclosure relates to semiconductor structures and, moreparticularly, to a symmetric tunnel field effect transistor and methodsof manufacture.

BACKGROUND

Integrated Tunnel FETs (TFETs) are devices in which the gate controlsthe tunneling currents to the drain. TFETs are known to exhibit steepsubthreshold slope and temperature independent operation, which makesthe device suitable for low voltage applications.

Symmetric TFETs have some disadvantages, though. For example, symmetricTFETs have low ON current because of a long conduction path. They alsoexhibit increased junction capacitance. Also, in certain types of TFETswith a TSi-pad, there may be a high OFF current if the TSi-pad is notlightly doped. This, in turn, increases the series resistance of thedevice. Moreover, OFF state leakage may be an issue if band-gapengineering is not done properly.

SUMMARY

In an aspect of the disclosure, a structure comprises a gate structureincluding a source region and a drain region both of which comprise adoped VO₂ region.

In an aspect of the disclosure, a structure comprises a gate structure,an epitaxially grown source region on a first side of the gatestructure, and an epitaxially grown drain region on a second side of thegate structure. The epitaxially grown source region and drain regioncomprises a VO₂ region doped with chromium.

In an aspect of the disclosure, a method comprises: depositing doped VO₂region on a source side and a drain side of a device; and epitaxiallygrowing semiconductor material for a source region and a drain region onthe source side and the drain side of the device, respectively.

BRIEF DESCRIPTION OF THE DRAWINGS

The present disclosure is described in the detailed description whichfollows, in reference to the noted plurality of drawings by way ofnon-limiting examples of exemplary embodiments of the presentdisclosure.

FIG. 1 shows a symmetric tunnel field effect transistor (TFET) andfabrication processes in accordance with aspects of the presentdisclosure.

FIG. 2 shows a graph of field dependence of critical switchingtemperatures for a transition metal used in the TFET in accordance withaspects of the present disclosure.

FIG. 3 shows electrical fields in an ON state and OFF state of thesymmetric TFET of FIG. 1, in accordance with aspects of the presentdisclosure.

FIGS. 4a and 4b show current flows in the symmetric TFET of FIG. 1, inaccordance with aspects of the present disclosure.

DETAILED DESCRIPTION

The present disclosure relates to semiconductor structures and, moreparticularly, to a symmetric tunnel field effect transistor (TFET) andmethods of manufacture. More specifically, the symmetric TFET includes asource region and a drain region with a transition material and sametype doping. In embodiments, the source region and drain region can bedoped VO₂ to enable increased conduction. In embodiments, VO₂ can bedoped with Chromium or other transition metals. The symmetric TFET canbe implemented in FinFET and nanowire architectures.

The symmetric TFET of the present disclosure can be manufactured in anumber of ways using a number of different tools. In general, though,the methodologies and tools are used to form structures with dimensionsin the micrometer and nanometer scale. The methodologies, i.e.,technologies, employed to manufacture the symmetric TFET structures havebeen adopted from integrated circuit (IC) technology. For example, thestructures disclosed herein are built on wafers and are realized infilms of material patterned by photolithographic processes on the top ofa wafer. In particular, the fabrication of the symmetric TFET uses threebasic building blocks: (i) deposition of thin films of material on asubstrate, (ii) applying a patterned mask on top of the films byphotolithographic imaging, and (iii) etching the films selectively tothe mask.

FIG. 1 shows a symmetric TFET and fabrication processes in accordancewith aspects of the present disclosure. More specifically, the structure5 shown in FIG. 1 includes silicon on insulator (SOI) wafer 10,comprising a wafer 12, an insulator material 14 and semiconductormaterial patterned into a plurality of fins 16. In embodiments, thesemiconductor material may be composed of any suitable semiconductormaterial including, but not limited to, Si, SiGe, SiGeC, SiC, Ge alloys,GaAs, InAs, InP, or heterojunctions with III-V materials.

In embodiments, the plurality of fins 16 can be formed usingconventional lithography and etching processes. For example, theplurality of fins 16 can be formed using sidewall image transfer (SIT)techniques. In the SIT technique, for example, a mandrel is formed onthe semiconductor material, using conventional deposition, lithographyand etching processes. In an example of a SIT technique, the mandrelmaterial can be, e.g., SiO₂, deposited using conventional chemical vapordeposition (CVD) processes. A resist is formed on the mandrel material,and exposed to light to form a pattern (openings). A reactive ionetching is performed through the openings to form the mandrels. Inembodiments, the mandrels can have different widths and/or spacingdepending on the desired dimensions between the plurality of fins 16.Spacers are formed on the sidewalls of the mandrels which are preferablymaterial that is different than the mandrels, and which are formed usingconventional deposition processes known to those of skill in the art.The spacers can have a width which matches the dimensions of theplurality of fins 14, for example. The mandrels are removed or strippedusing a conventional etching process, selective to the mandrel material.An etching is then performed within the spacing of the spacers to formthe sub-lithographic features. The sidewall spacers can then bestripped. In embodiments, the plurality of fins 16 can be further etchedin order to tune the device.

Still referring to FIG. 1, doped VO₂ regions 18 are deposited in thesource region 20 a and drain region 20 b using conventional plasmaenhanced CVD (PECVD) processes. In the embodiments, the doped VO₂regions 18 can also be deposited by atomic layer deposition (ALD). Inembodiments, the VO₂ regions 18 are doped with Chromium and/or othertransition metals. The source region 20 a and drain region 20 b are thencompleted by epitaxially growing semiconductor material with either ap-type or n-type dopant. In embodiments, the semiconductor material canbe, e.g., Si/Ge, Si/SiGe or heterojunctions with III-V materials. Aworkfunction metal 22, gate dielectric material 24, spacer material 26,and gate structure 26 a can be formed using conventional deposition,lithography and etching (i.e., reactive ion etching (RIE)) processes, asshould be known to those of skill in the art such that no furtherdiscussion is required for a complete understanding of the invention.

In accordance with the above fabrication processes, a symmetric TFET isformed, with the source region 20 a and the drain region 20 b bothcomprising epitaxially grown semiconductor material and doped VO₂regions 18. It should also be understood by those of skill in the artthat similar processes can be used to form nanowire architectures, withthe doped VO₂ regions 18. In embodiments, the doped VO₂ regions 18 caninclude trivalent cations (e.g., Cr₃+ and/or Al₃+) to increase thetransition temperature of VO₂, and can also be doped VO₂, e.g., 1.1% W,to bring the transition temperature to room temperature.

FIG. 2 shows a graph of field dependence of critical switchingtemperatures for a transition metal, e.g., VO₂. This graph is providedto show the critical switching temperature of VO₂ at room temperature,e.g., 300K. Specifically, it is shown from the graph of FIG. 2 that VO₂exhibits phase transition at an electric field of about 0.1 E×10⁻⁶,V/cm. This data can be used to determine the electric fields in the ONstate and the OFF state as shown in FIG. 3 in order determine transitionstates, e.g., insulator or metal, of the doped VO₂ at room temperature.

Prior to discussing the electric fields in the ON state and the OFFstate as shown in FIG. 3, it is noteworthy to mention the resistance ofdoped VO₂ will abruptly increase at a certain transition temperature,e.g., 340° K. That is, after this transition temperature, the doped VO₂will act as an insulator. Moreover, doped VO₂ exhibits the followingcharacteristics/properties, amongst others, that are advantageous to thepresent application.

-   -   (i) Doped VO₂ acts as a high band gap insulator at room        temperature;    -   (ii) Doped VO₂ exhibits changes in electrical conductivity up to        5 order of magnitude;    -   (iii) Doped VO₂ exhibits switching time on the order of 5 ps;    -   (v) Doped VO₂ exhibits a latent heat of transition favorably        with the power dissipation in a single CMOS switching event,        e.g., 0.1 eV at 103 cal/mol;    -   (vi) The transition temperature of VO₂ may be decreased by the        addition of high-valent transition metals such as niobium,        molybdenum or tungsten;    -   (vii) Trivalent cations (Cr₃+ and Al₃+) increase the transition        temperature of VO₂;    -   (viii) A change in the transition temperature is exhibited by        doping VO₂, e.g., 1.1% W doping brings the transition        temperature down to room temperature; and    -   (ix) The transition temperature of doped VO₂ can be decreased by        applying an electric field.

FIG. 3 shows electrical fields in the ON state and OFF state of thesymmetric TFET of FIG. 1 in accordance with aspects of the presentdisclosure. In particular, as shown in FIG. 3, with the drain at a highpotential, e.g., 0.5V, in both an ON state and OFF state, doped VO₂ inthe drain region 20 b will transition to a metal and the doped VO₂ inthe source region 20 a will transition to an insulator. Advantageously,in the ON state, the drain region 20 b is less resistive and thereforeexhibits a high ON state current.

FIGS. 4a and 4b show current flows in the symmetric TFET of FIG. 1. Morespecifically, FIG. 4a schematically shows a current flowing from thesource region 20 a to the drain region 20 b. FIG. 4b , though,schematically shows a current flowing in the opposite direction as shownin FIG. 4a . In other words, the source region 20 a of the structure canact as a drain and the drain region 20 b can act as a source, dependingon the application of Vdd. Accordingly, in the symmetric TFET of thepresent invention, the source region and the drain region areinterchangeable based on the application of Vdd.

The method(s) as described above is used in the fabrication ofintegrated circuit chips. The resulting integrated circuit chips can bedistributed by the fabricator in raw wafer form (that is, as a singlewafer that has multiple unpackaged chips), as a bare die, or in apackaged form. In the latter case the chip is mounted in a single chippackage (such as a plastic carrier, with leads that are affixed to amotherboard or other higher level carrier) or in a multichip package(such as a ceramic carrier that has either or both surfaceinterconnections or buried interconnections). In any case the chip isthen integrated with other chips, discrete circuit elements, and/orother signal processing devices as part of either (a) an intermediateproduct, such as a motherboard, or (b) an end product. The end productcan be any product that includes integrated circuit chips, ranging fromtoys and other low-end applications to advanced computer products havinga display, a keyboard or other input device, and a central processor.

The descriptions of the various embodiments of the present disclosurehave been presented for purposes of illustration, but are not intendedto be exhaustive or limited to the embodiments disclosed. Manymodifications and variations will be apparent to those of ordinary skillin the art without departing from the scope and spirit of the describedembodiments. The terminology used herein was chosen to best explain theprinciples of the embodiments, the practical application or technicalimprovement over technologies found in the marketplace, or to enableothers of ordinary skill in the art to understand the embodimentsdisclosed herein.

What is claimed:
 1. A structure comprising a field effect transistorcomprising a gate structure and a source region and a drain region bothof which comprise a doped VO₂ region, wherein the doped VO₂ regionincludes tungsten.
 2. The structure of claim 1, wherein the structure isa symmetric tunnel field effect transistor comprising the source regionand the drain region with same type dopants.
 3. The structure of claim1, wherein the structure is a finFET symmetric tunnel field effecttransistor.
 4. The structure of claim 1, wherein the doped VO₂ region isa p-type or a n-type dopant.
 5. The structure of claim 1, wherein thesource region and the drain region comprise epitaxially grown Si/Ge. 6.The structure of claim 1, wherein the source region and the drain regioncomprise epitaxially grown Si/SiGe.
 7. The structure of claim 1, whereinthe doped VO₂ region comprises Cr₃+.
 8. The structure of claim 1,wherein the doped VO₂ region comprises Al₃+.
 9. The structure of claim1, wherein the source region and the drain region comprise epitaxiallygrown heterojunctions with III-V materials.